Analysis of the $D{\bar{D}}^{\ast }K$ system with QCD sum rules

Abstract

In this article, we construct the color singlet-singlet-singlet interpolating current with $I\left(J^P\right)=\frac{3}{2}\left(1^{-}\right)$ to study the $D{\bar{D}}^{\ast }K$ system through QCD sum rules approach. In calculations, we consider the contributions of the vacuum condensates up to dimension-16 and employ the formula $\mu =\sqrt{M_{X/Y/Z}^2-{\left(2{\mathbb{M}}_c\right)}^2}$ to choose the optimal energy scale of the QCD spectral density. The numerical result $M_Z=4.71_{-0.11}^{+0.19}\mathrm{GeV}$ indicates that there exists a resonance state $Z$ lying above the $D{\bar{D}}^{\ast }K$ threshold to saturate the QCD sum rules. This resonance state $Z$ may be found by focusing on the channel $J/\psi \pi K$ of the decay $B⟶J/\psi \pi \pi K$ in the future.

arXiv comment9 pages, 4 figures

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Cited by in corpus (4)

• Analysis of the tetraquark and hexaquark molecular states with the QCD sum rules
• Production of the (predicted) $K^{\ast }(4307)$ in $B$ decays
• Electromagnetic properties of the $D{\bar{D}}^{\ast }K$ molecular hexaquark state
• Spectrum of Light Hexaquark States in Triquark-antitriquark Configuration